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Laser-wakefield accelerators for high-resolution X-ray imaging of complex microstructures.
Hussein, A E; Senabulya, N; Ma, Y; Streeter, M J V; Kettle, B; Dann, S J D; Albert, F; Bourgeois, N; Cipiccia, S; Cole, J M; Finlay, O; Gerstmayr, E; González, I Gallardo; Higginbotham, A; Jaroszynski, D A; Falk, K; Krushelnick, K; Lemos, N; Lopes, N C; Lumsdon, C; Lundh, O; Mangles, S P D; Najmudin, Z; Rajeev, P P; Schlepütz, C M; Shahzad, M; Smid, M; Spesyvtsev, R; Symes, D R; Vieux, G; Willingale, L; Wood, J C; Shahani, A J; Thomas, A G R.
  • Hussein AE; Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, 48109-2099, USA. aehuss@umich.edu.
  • Senabulya N; Department of Materials Science and Engineering, University of Michigan, Ann Arbor, MI, 48109-2099, USA.
  • Ma Y; Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, 48109-2099, USA.
  • Streeter MJV; Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.
  • Kettle B; The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.
  • Dann SJD; Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.
  • Albert F; The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.
  • Bourgeois N; The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK.
  • Cipiccia S; The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK.
  • Cole JM; Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.
  • Finlay O; The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.
  • Gerstmayr E; Lawrence Livermore National Laboratory, NIF and Photon Sciences, Livermore, CA, 94550, USA.
  • González IG; Central Laser Facility, STFC Rutherford Appleton Laboratory, Didcot, OX11 0QX, UK.
  • Higginbotham A; Diamond Light Source, Harwell Science and Innovation Campus, Fermi Avenue, Didcot, OX11 0DE, UK.
  • Jaroszynski DA; The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK.
  • Falk K; Physics Department, Lancaster University, Lancaster, LA1 4YB, UK.
  • Krushelnick K; The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.
  • Lemos N; The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK.
  • Lopes NC; Department of Physics, Lund University, P.O. Box 118, S-22100, Lund, Sweden.
  • Lumsdon C; York Plasma Institute, Department of Physics, University of York, York, YO10 5DD, UK.
  • Lundh O; The Cockcroft Institute, Keckwick Lane, Daresbury, WA4 4AD, UK.
  • Mangles SPD; SUPA, Department of Physics, University of Strathclyde, Glasgow, G4 0NG, UK.
  • Najmudin Z; Helmholtz-Zentrum Dresden-Rossendorf, Bautzner Landstraße 400, 01328, Dresden, Germany.
  • Rajeev PP; Technische Universität Dresden, 01062, Dresden, Germany.
  • Schlepütz CM; Institute of Physics of the ASCR, 182 21, Prague, Czech Republic.
  • Shahzad M; Center for Ultrafast Optical Science, University of Michigan, Ann Arbor, MI, 48109-2099, USA.
  • Smid M; Lawrence Livermore National Laboratory, NIF and Photon Sciences, Livermore, CA, 94550, USA.
  • Spesyvtsev R; The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK.
  • Symes DR; GoLP/Instituto de Plasmas e Fusão Nuclear, Instituto Superior Técnico, U.L., Lisboa, 1049-001, Portugal.
  • Vieux G; York Plasma Institute, Department of Physics, University of York, York, YO10 5DD, UK.
  • Willingale L; Department of Physics, Lund University, P.O. Box 118, S-22100, Lund, Sweden.
  • Wood JC; The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK.
  • Shahani AJ; The John Adams Institute for Accelerator Science, Imperial College London, London, SW7 2AZ, UK.
  • Thomas AGR; Central Laser Facility, STFC Rutherford Appleton Laboratory, Didcot, OX11 0QX, UK.
Sci Rep ; 9(1): 3249, 2019 Mar 01.
Article en En | MEDLINE | ID: mdl-30824838
ABSTRACT
Laser-wakefield accelerators (LWFAs) are high acceleration-gradient plasma-based particle accelerators capable of producing ultra-relativistic electron beams. Within the strong focusing fields of the wakefield, accelerated electrons undergo betatron oscillations, emitting a bright pulse of X-rays with a micrometer-scale source size that may be used for imaging applications. Non-destructive X-ray phase contrast imaging and tomography of heterogeneous materials can provide insight into their processing, structure, and performance. To demonstrate the imaging capability of X-rays from an LWFA we have examined an irregular eutectic in the aluminum-silicon (Al-Si) system. The lamellar spacing of the Al-Si eutectic microstructure is on the order of a few micrometers, thus requiring high spatial resolution. We present comparisons between the sharpness and spatial resolution in phase contrast images of this eutectic alloy obtained via X-ray phase contrast imaging at the Swiss Light Source (SLS) synchrotron and X-ray projection microscopy via an LWFA source. An upper bound on the resolving power of 2.7 ± 0.3 µm of the LWFA source in this experiment was measured. These results indicate that betatron X-rays from laser wakefield acceleration can provide an alternative to conventional synchrotron sources for high resolution imaging of eutectics and, more broadly, complex microstructures.